An Improved Third-Order WENO-Z Scheme

In this paper, we develop an improved third-order WENO-Z scheme. Firstly, a new reference smoothness indicator is derived by slightly modifying that of WENO-N3 scheme proposed by Wu and Zhang (Int. J. Numer. Meth. Fl. 78:162–187, 2015). Then a new term is added to the weights of the developed scheme to further slightly increase the weight of less-smooth stencil. Some numerical experiments are provided to demonstrate that the improved scheme is stable and significantly outperforms the conventional third-order WENO scheme of Jiang and Shu, while providing essentially non-oscillatory solutions near strong discontinuities.

[1]  Gecheng Zha,et al.  Improvement of weighted essentially non-oscillatory schemes near discontinuities , 2009 .

[2]  P. Woodward,et al.  The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .

[3]  Wai-Sun Don,et al.  An improved weighted essentially non-oscillatory scheme for hyperbolic conservation laws , 2008, J. Comput. Phys..

[4]  Bruno Costa,et al.  An improved WENO-Z scheme , 2016, J. Comput. Phys..

[5]  Jianhan Liang,et al.  A new smoothness indicator for third‐order WENO scheme , 2016 .

[6]  J. M. Powers,et al.  Mapped weighted essentially non-oscillatory schemes: Achieving optimal order near critical points , 2005 .

[7]  S. Osher,et al.  Weighted essentially non-oscillatory schemes , 1994 .

[8]  Yeon Ju Lee,et al.  An improved weighted essentially non-oscillatory scheme with a new smoothness indicator , 2013, J. Comput. Phys..

[9]  Yong-Tao Zhang,et al.  Resolution of high order WENO schemes for complicated flow structures , 2003 .

[10]  P. Lax Weak solutions of nonlinear hyperbolic equations and their numerical computation , 1954 .

[11]  Jungho Yoon,et al.  Modified Non-linear Weights for Fifth-Order Weighted Essentially Non-oscillatory Schemes , 2016, J. Sci. Comput..

[12]  Nail K. Yamaleev,et al.  Third-order Energy Stable WENO scheme , 2008, J. Comput. Phys..

[13]  Xu-Dong Liu,et al.  Solution of Two-Dimensional Riemann Problems of Gas Dynamics by Positive Schemes , 1998, SIAM J. Sci. Comput..

[14]  Naga Raju Gande,et al.  Third‐order WENO scheme with a new smoothness indicator , 2017 .

[15]  Jianxian Qiu,et al.  Finite Difference Hermite WENO Schemes for Hyperbolic Conservation Laws , 2014, Journal of Scientific Computing.

[16]  Zhao Yuxin,et al.  A high‐resolution hybrid scheme for hyperbolic conservation laws , 2015 .

[17]  G. Sod A survey of several finite difference methods for systems of nonlinear hyperbolic conservation laws , 1978 .

[18]  Wai-Sun Don,et al.  Accuracy of the weighted essentially non-oscillatory conservative finite difference schemes , 2013, J. Comput. Phys..

[19]  Chi-Wang Shu,et al.  Efficient Implementation of Weighted ENO Schemes , 1995 .

[20]  Wai-Sun Don,et al.  High order weighted essentially non-oscillatory WENO-Z schemes for hyperbolic conservation laws , 2011, J. Comput. Phys..

[21]  Feng Qu,et al.  An efficient adaptive high-order scheme based on the WENO process , 2016 .